CN108169208A - A kind of Raman spectrum detector calibration method - Google Patents

A kind of Raman spectrum detector calibration method Download PDF

Info

Publication number
CN108169208A
CN108169208A CN201810046148.7A CN201810046148A CN108169208A CN 108169208 A CN108169208 A CN 108169208A CN 201810046148 A CN201810046148 A CN 201810046148A CN 108169208 A CN108169208 A CN 108169208A
Authority
CN
China
Prior art keywords
offset
spectrum
raman spectrum
difference
calibration method
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201810046148.7A
Other languages
Chinese (zh)
Other versions
CN108169208B (en
Inventor
徐晓轩
王斌
文虹镜
时金蒙
车颖
梁菁
徐阳阳
杨江涛
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nankai University
Original Assignee
Nankai University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nankai University filed Critical Nankai University
Priority to CN201810046148.7A priority Critical patent/CN108169208B/en
Publication of CN108169208A publication Critical patent/CN108169208A/en
Application granted granted Critical
Publication of CN108169208B publication Critical patent/CN108169208B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65Raman scattering
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/01Arrangements or apparatus for facilitating the optical investigation

Landscapes

  • Health & Medical Sciences (AREA)
  • General Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
  • Spectrometry And Color Measurement (AREA)

Abstract

A kind of Raman spectrum detector calibration method, including following operating procedure, step 1 obtains reference spectra S1;Step 2 obtains initial spectrum S2;Step 3 obtains current background spectrum S3;Step 4, calculate the first difference spectrum Sd1 of the reference spectra S1 and the initial spectrum S2, the second difference spectrum Sd2 of the reference spectra S1 and current background spectrum S3 are calculated, calculates the third difference spectrum Sd3 of the initial spectrum S2 and the current background spectrum S3;Step 5 determines the first offset △ v1 and the second offset △ v2;Step 6 is modified the Raman spectrum of testing result using the first offset △ v1 or the Raman spectrum of testing result is modified using the 4th offset △ v4.The present invention possesses calibration with reference to the advantages of more, calibration degree is high, and real-time is good.

Description

A kind of Raman spectrum detector calibration method
Technical field
The present invention relates to Raman spectrum detection technique fields, and in particular to a kind of Raman spectrum detector calibration method.
Background technology
The wavelength of the laser of Raman spectrometer is typically when laser dispatches from the factory or when Raman spectrometer dispatches from the factory into rower Location survey amount has determined that.But the wavelength of laser can be because small drift occurs for environment temperature, the fluctuation etc. of electronic circuit.Using Laser on Raman spectrometer is usually higher to the stability requirement of optical maser wavelength, it is desirable that ± 2cm-1 or higher are stablized Property parameter directly affects the Raman shifts measurement accuracy of instrument.In long-time service, environmental change, long-distance after Raman spectrometer manufacture Its optical maser wavelength is waited to be likely to occur drift after transport, it will usually be modified by modes such as self calibrations to optical maser wavelength. Common method for self-calibrating is:Measure the Raman spectrum of certain standard substance (such as polystyrene), and with the mark of the standard substance Quasi- spectrogram is compared, and then learns the offset of optical maser wavelength.The shortcomings that existing self-alignment method, is do not have Real-time can only give a constant correction value, and self-alignment condition is carried out under what state and is difficult to hold.
Invention content
The object of the present invention is to provide a kind of Raman spectrum detector calibration methods, and present invention offer is a kind of quickly to be carried out The method for carrying out field calibration.
The present invention above-mentioned technical purpose technical scheme is that:A kind of Raman spectrum detector school Quasi- method, including following operating procedure,
Step 1 carries out standard reference material using Raman spectrum detector the signal sampling of T time section, obtains reference light Compose S1;
Step 2 using Raman spectrum detector to being carried out the signal sampling of the T time section by object to be detected, obtains just Beginning spectrum S2;
Step 3 carries out vacant sample cell using Raman spectrum detector the signal sampling of the T time section, obtains Current background spectrum S3;
Step 4 calculates the first difference spectrum Sd1 of the reference spectra S1 and the initial spectrum S2, calculates the ginseng The second difference spectrum Sd2 of spectrum S1 and current background spectrum S3 are examined, calculates the initial spectrum S2 and the current background light Compose the third difference spectrum Sd3 of S3;
Step 5 determines that reference laser is composed according to the second difference spectrum Sd2 and the third difference spectrum Sd3 respectively Peak with by object laser spectral peak to be checked, respectively according to the center of the reference laser spectral peak and the object laser spectral peak to be checked point It Que Ding not the first offset △ v1 and the second offset △ v2;
Step 6, the first offset △ v1 and the second offset △ v2, using described the if equal One offset △ v1 are modified the Raman spectrum of testing result;It is true according to the first difference spectrum Sd1 if unequal Determine difference laser spectral peak, third offset △ v3 are then determined according to the center of the difference laser spectral peak, using described Third offset △ v3 are modified to obtain the 4th offset △ v4 to the offset △ v1, finally using the described 4th offset Amount △ v4 are modified the Raman spectrum of testing result.
The first offset △ v1 will be used to join the standard as a preference of the present invention, the step 5 further includes The testing result vf for examining object is directly modified, and the 5th offset is obtained after correction result and standard Raman spectroscopy are compared △ v5 are measured, the first offset △ v1 and the second offset △ v2 are modified using the 5th offset △ v5 Obtain final first offset △ v1aWith final second offset △ v2a, use the final first offset △ v1aWith it is described Final second offset △ v2aStep 6 behaviour is carried out after replacing the first offset △ v1 and the second offset △ v2 Make.
As a preference of the present invention, the optical density parameter of the notch filtering light piece of the Raman spectrum detector for 6.5~ 7.5。
As a preference of the present invention, first it is placed in dark place before being additionally included in the operation for carrying out the step one~step 6 The step 1~step 6 is inside first carried out in advance carries out preposition calibration.
As a preference of the present invention, one~step 6 of the step of preposition calibration is further included and is provided using standard incandescent lamp Bias light has carried out luminous environment preliminary calibration.
As a preference of the present invention, when the second offset △ v2 are 0 value, without correcting in the step six Directly export result.
As a preference of the present invention, when the first offset △ v1 are 0 value, directly using described in the step 6 Second offset △ v2 are modified the Raman spectrum of testing result.
As a preference of the present invention, the standard reference material is polystyrene.
In conclusion the present invention has the advantages that:
The present invention possesses calibration with reference to the advantages of more, calibration degree is high, and real-time is good.
Description of the drawings
Fig. 1 is the operational flowchart of the embodiment of the present invention.
Specific embodiment
The present invention is described in further detail below in conjunction with attached drawing.
As shown in Figure 1, the first embodiment of the present invention includes following operating procedure,
Step 1 carries out standard reference material using Raman spectrum detector the unified testing time T time section of standard Signal sampling obtains reference spectra S1, and wherein standard reference material is polystyrene, the notch filtering light piece of Raman spectrum detector Optical density parameter is 6.5~7.5;
Step 2, using Raman spectrum detector to by object to be detected carry out T time section signal sampling, obtain initial light Compose S2;
Step 3 carries out vacant sample cell using Raman spectrum detector the signal sampling of T time section, obtains current Background spectrum S3;
Step 4 calculates the first difference spectrum Sd1 of reference spectra S1 and initial spectrum S2, calculates reference spectra S1 with working as The second difference spectrum Sd2 of preceding background spectrum S3 calculates the third difference spectrum of initial spectrum S2 and current background spectrum S3 Sd3;
Step 5 determines reference laser spectral peak with being treated according to the second difference spectrum Sd2 and third difference spectrum Sd3 respectively Object laser spectral peak is examined, double sampling mistake is determined according to the center of reference laser spectral peak and object laser spectral peak to be checked respectively respectively The first offset △ v1 and second between the reference laser wavelength that optical maser wavelength is provided with respect to Raman spectrum detector in journey are inclined Shifting amount △ v2;
Step 6 compares the first offset △ v1 and the second offset △ v2, and the first offset △ v1 are used if equal The Raman spectrum of testing result vi is modified, correcting mode is vi=vi+ △ v1;According to the first difference light if unequal Spectrum Sd1 determines difference laser spectral peak, then determines laser in reference substance sampling process according to the center of difference laser spectral peak Wavelength is with respect to the third offset △ v3 between optical maser wavelength in checking matter sampling process, using third offset △ v3 to offset Amount △ v1 are modified to obtain the 4th offset △ v4, finally using the 4th offset △ v4 to the Raman spectrum of testing result into Row is corrected, and correcting mode is vi=vi+ △ v4, in this step when the second offset △ v2 are 0 value, without repairing in step 6 Just directly export result.When the first offset △ v1 are 0 value, directly detection is tied using the second offset △ v2 in step 6 The Raman spectrum of fruit vi is modified.
Second of embodiment of the present invention is under the premise of all operationss step for keeping the first embodiment in step 5 Increase operation again, the operating method is will directly repair the testing result vf of standard reference material using the first offset △ v1 Just, and by correction result and standard Raman spectroscopy it is compared, normalized Raman of the standard Raman spectroscopy for theoretically polystyrene Spectrum obtains the 5th offset △ v5, using the 5th offset △ v5 to the first offset △ v1 and the second offset more afterwards △ v2 are modified to obtain final first offset △ v1aWith final second offset △ v2a, use final first offset △ v1aWith final second offset △ v2aStep 6 operation is carried out after replacing the first offset △ v1 and the second offset △ v2.
The embodiment of the present invention one is first placed in dark place in advance with embodiment two before the operation for carrying out step 1~step 6 It first carries out step 1~step 6 and carries out preposition calibration, the purpose of preposition calibration is that occur to eliminate manufacture before routine testing Error, preposition calibration must assure that △ v1~△ v5 are 0 value.The step of preposition calibration, one~step 6 was further included using warp Integrating sphere is crossed to carry out optical parameter test and reach standard sources required standard incandescent lamp providing at the beginning of bias light carried out luminous environment Step calibration, the step in order to generate that the offset under a standard luminous environment dispatches from the factory have luminous environment calibration.
This specific embodiment is only explanation of the invention, is not limitation of the present invention, people in the art Member can as needed make the present embodiment the modification of no creative contribution after this specification is read, but as long as at this It is all protected in the right of invention by Patent Law.

Claims (8)

1. a kind of Raman spectrum detector calibration method, it is characterised in that:Including following operating procedure,
Step 1 carries out standard reference material using Raman spectrum detector the signal sampling of T time section, obtains reference spectra S1;
Step 2 using Raman spectrum detector to being carried out the signal sampling of the T time section by object to be detected, obtains initial light Compose S2;
Step 3 carries out vacant sample cell using Raman spectrum detector the signal sampling of the T time section, obtains current Background spectrum S3;
Step 4 calculates the first difference spectrum Sd1 of the reference spectra S1 and the initial spectrum S2, calculates the reference light The second difference spectrum Sd2 of S1 and current background spectrum S3 is composed, calculates the initial spectrum S2 and the current background spectrum S3 Third difference spectrum Sd3;
Step 5, respectively according to the second difference spectrum Sd2 and the third difference spectrum Sd3 determine reference laser spectral peak with It is true according to the center difference of the reference laser spectral peak and the object laser spectral peak to be checked respectively by object laser spectral peak to be checked Fixed first offset △ v1 and the second offset △ v2;
Step 6, the first offset △ v1 and the second offset △ v2, if equal using described first partially Shifting amount △ v1 are modified the Raman spectrum of testing result;Difference is determined according to the first difference spectrum Sd1 if unequal It is worth laser spectral peak, third offset △ v3 is then determined according to the center of the difference laser spectral peak, use the third Offset △ v3 are modified to obtain the 4th offset △ v4 to the offset △ v1, finally using the 4th offset △ V4 is modified the Raman spectrum of testing result.
2. a kind of Raman spectrum detector calibration method according to claim 1, it is characterised in that:The step 5 is also wrapped Including will use the first offset △ v1 to be directly modified the testing result vf of the standard reference material, and be tied correcting Fruit obtains the 5th offset △ v5 after being compared with standard Raman spectroscopy, using the 5th offset △ v5 to described first Offset △ v1 and the second offset △ v2 are modified to obtain final first offset △ v1aWith final second offset △v2a, use the final first offset △ v1aWith the final second offset △ v2aReplace the first offset △ Step 6 operation is carried out after v1 and the second offset △ v2.
3. a kind of Raman spectrum detector calibration method according to claim 1, it is characterised in that:The Raman spectrum The optical density parameter of the notch filtering light piece of detector is 6.5~7.5.
4. a kind of Raman spectrum detector calibration method according to claim 1, it is characterised in that:It is additionally included in and carries out institute It is first placed in dark place before the operation of one~step 6 of the step of stating and first carries out the step 1~preposition school of step 6 progress in advance It is accurate.
5. a kind of Raman spectrum detector calibration method according to claim 4, it is characterised in that:The preposition calibration Step 1~step 6 is further included has carried out luminous environment preliminary calibration using standard incandescent lamp offer bias light.
6. a kind of Raman spectrum detector calibration method according to claim 1, it is characterised in that:When the described second offset When measuring △ v2 as 0 value, result is directly exported without correcting in the step six.
7. a kind of Raman spectrum detector calibration method according to claim 1, it is characterised in that:When the described first offset When measuring △ v1 as 0 value, directly the Raman spectrum of testing result is carried out using the second offset △ v2 in the step 6 It corrects.
8. a kind of Raman spectrum detector calibration method according to claim 1, it is characterised in that:The canonical reference Object is polystyrene.
CN201810046148.7A 2018-01-17 2018-01-17 Raman spectrum detector calibration method Active CN108169208B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810046148.7A CN108169208B (en) 2018-01-17 2018-01-17 Raman spectrum detector calibration method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810046148.7A CN108169208B (en) 2018-01-17 2018-01-17 Raman spectrum detector calibration method

Publications (2)

Publication Number Publication Date
CN108169208A true CN108169208A (en) 2018-06-15
CN108169208B CN108169208B (en) 2020-08-25

Family

ID=62514656

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810046148.7A Active CN108169208B (en) 2018-01-17 2018-01-17 Raman spectrum detector calibration method

Country Status (1)

Country Link
CN (1) CN108169208B (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1977152A (en) * 2004-06-30 2007-06-06 凯米映像公司 Method and apparatus for peak compensation in an optical filter
CN102608095A (en) * 2010-06-25 2012-07-25 清华大学 Method for automatically calibrating Raman spectrum detection system by utilizing standard sample
CN106596499A (en) * 2016-11-01 2017-04-26 北京华泰诺安技术有限公司 Real-time Raman spectrum calibration method

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1977152A (en) * 2004-06-30 2007-06-06 凯米映像公司 Method and apparatus for peak compensation in an optical filter
CN102608095A (en) * 2010-06-25 2012-07-25 清华大学 Method for automatically calibrating Raman spectrum detection system by utilizing standard sample
CN106596499A (en) * 2016-11-01 2017-04-26 北京华泰诺安技术有限公司 Real-time Raman spectrum calibration method

Also Published As

Publication number Publication date
CN108169208B (en) 2020-08-25

Similar Documents

Publication Publication Date Title
US4373818A (en) Method and device for analysis with color identification test paper
Kobulnicky et al. Measuring global galaxy metallicities using emission-line equivalent widths
JP6756709B2 (en) How to calibrate a spectroradiometer
CN106596613B (en) A method of road detection elements content is scanned using Xray fluorescence spectrometer
US20150142364A1 (en) Spectrometer reference calibration
EP2355164A1 (en) Solar battery evaluation device and method for evaluating solar battery
EP2841891A1 (en) Spectrometer secondary reference calibration
US20180224334A1 (en) High accuracy absorbance spectrophotometers
KR20080086063A (en) Combined sensor for detecting fault in a plasma process chamber incorporated with self plasma chamber
US20130194564A1 (en) Method and apparatus for measuring photovoltaic cells
JP2001153724A (en) Wavelength standard
US7145650B2 (en) Method of instrument standardization for a spectroscopic device
US20120194818A1 (en) Gas Analyzer for Measuring the Mercury Content of a Gas
Chan et al. Use of vertically resolved plasma emission as an indicator for flagging matrix effects and system drift in inductively coupled plasma-atomic emission spectrometry
CN108169208A (en) A kind of Raman spectrum detector calibration method
CN103116065B (en) A kind of method of testing of solar photovoltaic assembly power
US5065613A (en) Method for the direct presentation of a differential measured quantity in terms of its correct physical unit
CN112730304A (en) Infrared gas alarm and gas concentration detection method
CN110346346B (en) Raman gas detection method based on compressed sensing correlation algorithm
CN107402365B (en) Calibration method of LED photoelectric comprehensive tester
CN100414272C (en) Integrating light radiation degree measuring system and method with spectrum analysis correction
CN116929630A (en) Wide-range multi-parameter vacuum measurement device and method
CN108896511A (en) A kind of intelligent method for repairing the deformation of spectroanalysis instrument spectrogram
Castiglioni et al. Evaluation of instrumental errors built in circular dichroism spectrometers
Workman Jr First principles of instrument calibration

Legal Events

Date Code Title Description
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant